JPH076490Y2 - Electromagnetic flow meter - Google Patents

Electromagnetic flow meter

Info

Publication number
JPH076490Y2
JPH076490Y2 JP9079489U JP9079489U JPH076490Y2 JP H076490 Y2 JPH076490 Y2 JP H076490Y2 JP 9079489 U JP9079489 U JP 9079489U JP 9079489 U JP9079489 U JP 9079489U JP H076490 Y2 JPH076490 Y2 JP H076490Y2
Authority
JP
Japan
Prior art keywords
magnetic field
coil
measuring tube
core
tube
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP9079489U
Other languages
Japanese (ja)
Other versions
JPH0330825U (en
Inventor
義三 石田
千秋 岩佐
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP9079489U priority Critical patent/JPH076490Y2/en
Publication of JPH0330825U publication Critical patent/JPH0330825U/ja
Application granted granted Critical
Publication of JPH076490Y2 publication Critical patent/JPH076490Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【考案の詳細な説明】 (イ)産業上の利用分野 この考案は、電磁流量計に関する。[Detailed Description of the Invention] (a) Field of Industrial Application This invention relates to an electromagnetic flow meter.

(ロ)従来の技術 第4図及び第5図は、従来の電磁流量計を示す断面図で
ある。
(B) Conventional Technique FIGS. 4 and 5 are sectional views showing a conventional electromagnetic flowmeter.

この電磁流量計は、内周面にライニング層12を設けた非
磁性測定管1と、この測定管1の外側に設けられ、測定
管1の管軸に対し直交する磁界を発生させる磁界発生手
段(コア2にコイル3を捲回して成る磁界発生部)と、
測定管1の内壁に、測定管1の管軸及び磁界に対して直
交状に対向配備された一対の電極4、4aと、一端を電極
4(4a)に、他端を回路部7の端子部71に接続したリー
ド線41とから構成され、これら構成要素が内面にシール
ド板部81を備えた被覆体8で被覆されている。
This electromagnetic flowmeter comprises a non-magnetic measuring tube 1 provided with a lining layer 12 on its inner peripheral surface, and a magnetic field generating means provided outside the measuring tube 1 for generating a magnetic field orthogonal to the tube axis of the measuring tube 1. (A magnetic field generating portion formed by winding the coil 3 around the core 2),
On the inner wall of the measuring tube 1, a pair of electrodes 4 and 4a arranged to face each other orthogonally to the tube axis and the magnetic field of the measuring tube 1, one end to the electrode 4 (4a), and the other end to the terminal of the circuit section 7 And a lead wire 41 connected to the portion 71, and these components are covered with a cover 8 having a shield plate portion 81 on the inner surface.

測定管1の内部を、被測定流体が流れると、この流速に
対応して両電極4、4a間に電圧が発生する。この電圧を
リード線41で取り出すことで、被測定流体の流量を測定
する。
When the fluid to be measured flows inside the measuring tube 1, a voltage is generated between the electrodes 4 and 4a corresponding to this flow velocity. By extracting this voltage with the lead wire 41, the flow rate of the fluid to be measured is measured.

(ハ)考案が解決しようとする課題 上記、電磁流量計の磁界発生手段は、第4図で示すよう
に、測定管1の外周であって、両端フランジ部11、11間
に配備される。つまり、測定管1の管上周部と管下周部
に、励磁コイル3を捲回したコア2が、それぞれ対向状
に配備してある。この励磁コイル3は、コア2の外周面
に直接捲回配備されている。
(C) Problem to be Solved by the Invention The magnetic field generating means of the electromagnetic flowmeter is arranged on the outer circumference of the measuring tube 1 and between the flange portions 11, 11 at both ends, as shown in FIG. That is, the core 2 around which the exciting coil 3 is wound is provided in the upper peripheral portion and the lower peripheral portion of the measuring tube 1 so as to face each other. The exciting coil 3 is directly wound around the outer peripheral surface of the core 2.

近年、電磁流量計の小型化、特に管軸長さ(面間距離)
の短い測定管が要望されている。ところが、コアの外周
面にコイルを捲回した従来の構造のものにおいて、測定
管を短くするとコア及びコイルの幅(管軸方向の長さ)
が短くなる。この事は、管内での磁界発生領域が小さく
なり、また磁束密度が減少し、電極に生じる起電力が小
さくなる結果、測定感度が悪くなる。ところで、コイル
巻数を増やせば、充分な磁界発生領域を確保できると考
えられるが、幅の短いコアに対しコイル巻数を多くする
と結局コイル全体として太くなり、小型化要請に反する
こととなる。一方、励磁電流を大きくすることで、充分
な磁界領域を確保することも考えられる。つまり、流す
電流を大きくすれば磁束密度減少の問題は解決するが、
その分、消費電力が大となり、好ましくない。
In recent years, miniaturization of electromagnetic flowmeters, especially tube axis length (face-to-face distance)
A short measuring tube is required. However, in the conventional structure in which the coil is wound around the outer peripheral surface of the core, if the measuring tube is shortened, the width of the core and the coil (length in the tube axis direction)
Becomes shorter. This means that the magnetic field generation area in the tube is reduced, the magnetic flux density is reduced, and the electromotive force generated in the electrodes is reduced, resulting in poor measurement sensitivity. By the way, it is considered that a sufficient magnetic field generation region can be secured by increasing the number of coil turns. However, if the number of coil turns is increased with respect to a core having a short width, the coil as a whole becomes thicker, which is against the demand for size reduction. On the other hand, it is possible to secure a sufficient magnetic field region by increasing the exciting current. In other words, increasing the flowing current solves the problem of magnetic flux density reduction,
The power consumption increases accordingly, which is not preferable.

この結果、従来のようにコアの外周面に単にコイルを捲
回配備する構造のものでは、電磁流量計の小型化要請に
対応し得ない不利があった。
As a result, the conventional structure in which the coil is simply wound around the outer peripheral surface of the core cannot meet the demand for downsizing the electromagnetic flowmeter.

この考案は、以上のような課題を解消させ、使用便宜で
精度よく流量測定でき、且つ小型化を実現し得る電磁流
量計を提供することを目的とする。
It is an object of the present invention to solve the above problems, to provide an electromagnetic flow meter that can be used for convenience, can accurately measure a flow rate, and can be downsized.

(ニ)課題を解決するための手段及び作用 この目的を達成させるために、この考案の電磁流量計で
は、次のような構成としている。
(D) Means and Actions for Solving the Problem In order to achieve this object, the electromagnetic flowmeter of the present invention has the following configuration.

電磁流量計は、被測定流体が流れる非磁性の測定管と、
この測定管の外側に設けられ、測定管の管軸に対し直交
する磁界を発生させる磁界発生手段と、前記測定管の内
壁に、測定管の管軸及び磁界に対して直交状に対向配備
された少なくとも一対の電極とから成る電磁流量計であ
って、前記磁界発生手段は、コアの周面に所定深さ内方
向へへこむ凹陥部を一周形成し、この凹陥部に対し励磁
コイルを捲回配備してなることを特徴としている。
The electromagnetic flowmeter is a non-magnetic measuring tube through which the fluid to be measured flows.
A magnetic field generating means which is provided outside the measuring tube and generates a magnetic field orthogonal to the tube axis of the measuring tube, and an inner wall of the measuring tube, which are arranged to face each other in a direction orthogonal to the tube axis and the magnetic field of the measuring tube. An electromagnetic flowmeter comprising at least a pair of electrodes, wherein the magnetic field generating means forms a recess inwardly of a predetermined depth in the peripheral surface of the core, and an exciting coil is wound around the recess. It is characterized by being deployed.

このような構成を有する電磁流量計では、両端にフラン
ジ部を備えた測定管の管上周部と管下周部に、コイルを
捲回したコアがそれぞれ配備されている。このコアは、
測定管の曲率に対応した弯曲状で、周面に凹陥部を一周
形成してある。そして、この凹陥部に励磁コイルが捲回
してある。また、コアの幅(管軸方向の長さ)は、従来
の一般的なコアと同一に設定して充分な磁場の範囲が確
保されている。凹陥部にコイルを捲回配備することで、
コイル巻数が従来と同様であっても、凹陥部の深さ分だ
け、コイルの幅(管軸方向の長さ)が、従来のコイル幅
より短くなる。従って、測定管のフランジ間(面間距
離)を短く設定し得ることとなり、電磁流量計の小型化
を実現できる。
In the electromagnetic flowmeter having such a configuration, cores each having a coil wound are provided on the upper and lower peripheral portions of the measuring pipe having flange portions at both ends. This core is
It has a curved shape corresponding to the curvature of the measuring tube, and a concave portion is formed around the peripheral surface. An exciting coil is wound around the recess. Further, the width of the core (the length in the tube axis direction) is set to be the same as that of the conventional general core, and a sufficient magnetic field range is secured. By deploying the coil in the recess,
Even if the number of coil turns is the same as in the conventional case, the width of the coil (the length in the tube axis direction) becomes shorter than the conventional coil width by the depth of the recess. Therefore, the distance between the flanges (face-to-face distance) of the measuring pipe can be set short, and the electromagnetic flowmeter can be downsized.

(ホ)実施例 第1図及び第2図は、この考案に係る電磁流量計の具体
的な一実施例を示す断面図である。
(E) Embodiment FIG. 1 and FIG. 2 are sectional views showing a specific embodiment of the electromagnetic flowmeter according to the present invention.

電磁流量計は、公知のように、内周面にライニング層
(テフロン、ネオプレンゴム、ポリウレタン等の絶縁
層)12を設けた非磁性測定管1と、この測定管1の外側
に設けられ、測定管1の管軸に対し直交する磁界を発生
させる磁界発生手段(コア2にコイル3を捲回してなる
磁界発生部)と、測定管1の内壁に、測定管1の管軸及
び磁界に対して直交状に対向配備された一対の電極4、
4aと、一端を電極4(4a)に、他端を回路部7の回路端
子(端子部)71に接続したリード線(フレキシブルケー
ブル)41とから構成され、これらの構成要素が内面にシ
ールド板部81を備えた被覆体8で被覆されている。
As is well known, the electromagnetic flow meter is provided with a non-magnetic measuring tube 1 having a lining layer (an insulating layer made of Teflon, neoprene rubber, polyurethane, etc.) 12 on its inner peripheral surface, and a measuring tube 1 provided outside the measuring tube 1. A magnetic field generating means (a magnetic field generating part formed by winding the coil 3 around the core 2) for generating a magnetic field orthogonal to the tube axis of the tube 1, and an inner wall of the measuring tube 1 with respect to the tube axis and the magnetic field of the measuring tube 1. A pair of electrodes 4 arranged to face each other orthogonally,
4a and a lead wire (flexible cable) 41 having one end connected to the electrode 4 (4a) and the other end connected to the circuit terminal (terminal part) 71 of the circuit part 7, and these components are shielded on the inner surface. It is covered with a cover 8 having a portion 81.

上記磁界発生手段(コア2と、コア2の外周面に捲回さ
れたコイル3とから成る)は、測定管1の両端フランジ
部11間であって、測定管1の管上周部と管下周部とに、
それぞれ配備されている。
The magnetic field generating means (consisting of the core 2 and the coil 3 wound around the outer peripheral surface of the core 2) is provided between the flange portions 11 at both ends of the measuring pipe 1, and the upper peripheral portion of the measuring pipe 1 and the pipe. In the lower part,
Each is deployed.

この考案の特徴は、コア2の周面に凹陥部21を一周形成
し、この凹陥部21にコイル3を捲回配備した点にある。
The feature of this invention resides in that a concave portion 21 is formed around the peripheral surface of the core 2 and the coil 3 is wound around the concave portion 21.

コア2は、測定管1の曲率に対応した弯曲状(鞍型状)
で、周面に一定深さの凹陥部21を形成してある。実施例
では、第3図で示すように、コア2は厚み中央で上下に
2分割して、コア半体22a、2bを一対としている。そし
て、各半体2a、2bの上面外周をそれぞれ切欠き21a、21
b、各半体2a、2bを接面させた時、両切欠21a、21bによ
り凹陥部21が構成されるように設定している。また、こ
のコア2は、上下半体2a、2bの接面部に係合部、係合受
け部を設け、脱着可能に設定してある(図示せず)。
The core 2 has a curved shape (saddle shape) corresponding to the curvature of the measuring tube 1.
Thus, a concave portion 21 having a constant depth is formed on the peripheral surface. In the embodiment, as shown in FIG. 3, the core 2 is vertically divided into two parts at the center of thickness, and the core halves 22a and 2b are paired. Then, cutouts 21a, 21
b. When the half bodies 2a, 2b are brought into contact with each other, the recesses 21 are set by the notches 21a, 21b. Further, the core 2 is provided with engaging portions and engaging receiving portions on the contact surface portions of the upper and lower halves 2a and 2b so as to be detachable (not shown).

励磁コイル3は、上記凹陥部21に捲回されている。励磁
コイル3は、従来のものと同様で、巻数も同様に設定さ
れる。
The exciting coil 3 is wound around the recess 21. The exciting coil 3 is similar to the conventional one, and the number of turns is also set similarly.

このような構成を有する電磁流量計では、コア2の幅
(管軸方向の長さ)を、従来のコアの幅と同一に設定す
ることで、充分な磁場の範囲を確保できるようになって
いる。凹陥部21に対し、コイル3を捲回配備すること
で、コイル3の巻数が従来と同様であっても、凹陥部21
の深さ分だけ、コイル3の幅(管軸方向の長さ)が従来
のコイル幅よりも短くなる。従って、それだけ測定管1
の管軸長さ(両フランジ部11間の長さ)を短くでき、磁
界発生領域を縮小することなく、電磁流量計を小型化を
実現し得る。
In the electromagnetic flowmeter having such a configuration, by setting the width of the core 2 (the length in the tube axis direction) to be the same as the width of the conventional core, a sufficient magnetic field range can be secured. There is. By disposing the coil 3 around the recessed portion 21, even if the number of turns of the coil 3 is the same as the conventional one, the recessed portion 21
The width of the coil 3 (the length in the tube axis direction) becomes smaller than the conventional coil width by the depth. Therefore, that much measurement tube 1
The pipe axis length (the length between both flange portions 11) of can be shortened, and the electromagnetic flowmeter can be miniaturized without reducing the magnetic field generation region.

また、コア2は一対の上・下半体2a、2bを分離可能とし
た。従って、コイル3を取付ける場合は、コイル3を予
め所定の型により捲回して成形し、この成形したコイル
3に対し、分離したコア(上・下半体2a、2b)2を取付
ける(第3図参照)。これにより、コイル3とコア2と
の取付け作業が一層簡易となる。更に、コイル3を捲回
したコア2の一部が破損した場合等、コイル3に対し破
損した側の半体2a(2b)を、取り外し交換することが出
来る。
In addition, the core 2 can separate the pair of upper and lower halves 2a and 2b. Therefore, when the coil 3 is mounted, the coil 3 is preliminarily wound by a predetermined mold and molded, and the separated cores (upper and lower halves 2a, 2b) 2 are mounted on the molded coil 3 (third part). See figure). As a result, the work of attaching the coil 3 and the core 2 is further simplified. Further, when a part of the core 2 around which the coil 3 is wound is damaged, the half 2a (2b) on the damaged side of the coil 3 can be removed and replaced.

(ヘ)考案の効果 この考案では、以上のように、コアの周面に凹陥部を形
成し、この凹陥部にコイルを捲回配備することとしたか
ら、コアの幅(管軸方向の長さ)は従来のコア幅と同様
に設定して充分な磁場の範囲を確保すると共に、凹陥部
にコイルを捲回することで、凹陥部の深さ分だけコイル
の幅(管軸方向の長さ)を、従来のコイル幅より短くす
ることが出来る。従って、測定管の管軸長さ(面間距
離)を短く設定し得、電磁流量計の小型化を実現できる
等、考案目的を達成した優れた効果を有する。
(F) Effect of the device In this device, as described above, since the concave portion is formed on the peripheral surface of the core and the coil is wound around the concave portion, the width of the core (length in the axial direction of the pipe) Is set in the same manner as the conventional core width to secure a sufficient magnetic field range, and by winding the coil around the recess, the coil width (length in the axial direction of the tube) is increased by the depth of the recess. Can be made shorter than the conventional coil width. Therefore, the tube axial length (face-to-face distance) of the measuring tube can be set short, and the electromagnetic flowmeter can be downsized.

【図面の簡単な説明】[Brief description of drawings]

第1図は、実施例電磁流量計を示す管軸方向に平行に切
断した断面図、第2図は、同実施例電磁流量計の管軸に
直交する方向に切断した断面図、第3図は、実施例電磁
流量計のコアとコイルの関係を示す説明図、第4図は、
従来の電磁流量計を示す管軸方向に切断した断面図、第
5図は、従来の電磁流量計の管軸に直交する方向に切断
した断面図である。 1:測定管、2:コア、3:コイル、4・4a:電極、21:凹陥
部。
FIG. 1 is a cross-sectional view showing an electromagnetic flowmeter of the embodiment cut in parallel with a pipe axis direction, and FIG. 2 is a cross-sectional view taken in a direction orthogonal to the pipe axis of the electromagnetic flowmeter of the embodiment, FIG. Is an explanatory view showing the relationship between the core and the coil of the embodiment electromagnetic flowmeter, and FIG.
FIG. 5 is a cross-sectional view showing a conventional electromagnetic flow meter taken along the tube axis, and FIG. 5 is a cross-sectional view taken along the direction perpendicular to the tube axis of the conventional electromagnetic flow meter. 1: Measuring tube, 2: Core, 3: Coil, 4 ・ 4a: Electrode, 21: Recessed part.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】被測定流体が流れる非磁性の測定管と、こ
の測定管の外側に設けられ、測定管の管軸に対し直交す
る磁界を発生させる磁界発生手段と、前記測定管の内壁
に、測定管の管軸及び磁界に対して直交状に対向配備さ
れた少なくとも一対の電極とから成る電磁流量計におい
て、 前記磁界発生手段は、コアの周面に所定深さ内方向へへ
こむ凹陥部を一周形成し、この凹陥部に対し励磁コイル
を捲回配備してなることを特徴とする電磁流量計。
1. A non-magnetic measuring tube through which a fluid to be measured flows, magnetic field generating means provided outside the measuring tube for generating a magnetic field orthogonal to the tube axis of the measuring tube, and an inner wall of the measuring tube. An electromagnetic flowmeter comprising at least a pair of electrodes arranged to face each other in a direction orthogonal to the tube axis of the measuring tube and the magnetic field, wherein the magnetic field generating means is a concave portion that is recessed inward at a predetermined depth on the peripheral surface of the core. The electromagnetic flowmeter is characterized in that an exciting coil is wound around the recessed portion to form one round.
JP9079489U 1989-07-31 1989-07-31 Electromagnetic flow meter Expired - Lifetime JPH076490Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9079489U JPH076490Y2 (en) 1989-07-31 1989-07-31 Electromagnetic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9079489U JPH076490Y2 (en) 1989-07-31 1989-07-31 Electromagnetic flow meter

Publications (2)

Publication Number Publication Date
JPH0330825U JPH0330825U (en) 1991-03-26
JPH076490Y2 true JPH076490Y2 (en) 1995-02-15

Family

ID=31640307

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9079489U Expired - Lifetime JPH076490Y2 (en) 1989-07-31 1989-07-31 Electromagnetic flow meter

Country Status (1)

Country Link
JP (1) JPH076490Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0628638U (en) * 1992-09-16 1994-04-15 矢崎総業株式会社 Vehicle instrument

Also Published As

Publication number Publication date
JPH0330825U (en) 1991-03-26

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